Mn-Zn ferrite and production process thereof

ABSTRACT

The present invention provides a Mn—Zn ferrite having an electrical resistivity exceeding 1 Ωm order and having a high initial permeability of 4000 or more at 100 kHz and 100 or more at 10 MHz. The main components of the Mn—Zn ferrite include 44.0 to 49.8 mol % Fe 2 O 3 , 15.0 to 26.5 mol % ZnO, 0.1 to 3.0 mol % CoO, 0.02 to 1.00 mol % Mn 2 O 3 , and the remainder MnO. The Mn—Zn ferrite can be used in a wide frequency region of 100 kHz to 10 MHz by limiting Fe 2 O 3  content to a range of less than 50 mol %, that is the stoichiometric composition, inhibiting formation of Mn 2 O 3  and adding a proper amount of CoO.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an oxide magnetic material having soft magnetism, and more particularly relates to a Mn—Zn ferrite suitable for use as various inductance elements, impedance elements for EMI countermeasures and the like, and to a production process thereof.

2. Description of the Related Art

Typical oxide magnetic materials having soft magnetism include a Mn—Zn ferrite. Conventionally, this Mn—Zn ferrite usually has a basic component composition containing 52 to 55 mol % Fe₂O₃ on the average exceeding 50 mol %, which is the stoichiometric composition, 10 to 24 mol % ZnO and the remainder MnO. The Mn—Zn ferrite is usually produced by mixing respective material powders of Fe₂O₃ZnO and MnO in a prescribed ratio, subjecting mixed powders to respective steps of calcination, milling, component adjustment, granulation and pressing to obtain a desired shape, then conducting sintering treatment at 1200 to 1400° C. for 2 to 4 hours in a reducing atmosphere in which a relative partial pressure of oxygen is controlled to a low level by supplying nitrogen. The reason why the Mn—Zn ferrite is sintered in the reducing atmosphere is that Fe²⁺ is formed as the result of reducing a part of Fe³ ⁺. This Fe2+ has positive crystal magnetic anisotropy and cancels out negative crystal magnetic anisotropy of Fe³ to thereby enhance soft magnetism.

Amount of the above-mentioned Fe²⁺ formed depends on relative partial pressures of oxygen in sintering and cooling after the sintering. Therefore, when the relative partial pressure of oxygen is improperly set, it becomes difficult to ensure excellent soft magnetic properties. Thus, conventionally, the following expression (1) has been experimentally established and the relative partial pressure of oxygen in sintering and in cooling after the sintering has been controlled strictly in accordance with this expression (1).

log Po ₂=−14540/(T+273)+b  (1)

where T is temperature (° C.), Po₂ is a relative partial pressure of oxygen, and b is a constant, which is usually set at 7 to 8. The fact that the constant b is 7 to 8 means that the relative partial pressure of oxygen in the sintering must be controlled in a narrow range, which makes the sintering treatment very troublesome, thereby increasing production costs.

Additionally, in recent years, with miniaturization and performance improvement of electronic equipments there is an increasing tendency that signals are processed at a higher frequency. Thus, a magnetic material having excellent magnetic properties even in a higher frequency region as well has been needed.

However, when the Mn—Zn ferrite is used as a magnetic core material, an eddy current flows in a higher frequency region applied resulting in a larger loss. Therefore, in order to extend an upper limit of the frequency at which the Mn—Zn ferrite can be used as a magnetic core material, an electrical resistivity thereof must be made as high as possible. However, since the above-mentioned general Mn—Zn ferrite contains Fe₂O₃ in an amount larger than 50 mol % which is the stoichiometric composition, a large amount of Fe 2+ ions are present, thereby making the transfer of electrons between the above-mentioned Fe3+ and Fe²⁺ ions easy. Thus, the electrical resistivity of the Mn—Zn ferrite is in the order of 1 Ωm or less. Accordingly, an applicable frequency is limited to about several hundreds kHz at highest, and in a frequency region exceeding the limit, permeability (initial permeability) is significantly lowered to take away properties of the soft magnetic material.

In order to increase an apparent resistance of the Mn—Zn ferrite, in some cases, CaO, SiO₂ or the like is added as additive to impart a higher resistance to grain boundaries and at the same time the Mn—Zn ferrite is sintered at as low as about 1200° C. to diminish the grain size from its usual dimension, about 20 μm, to 5 μm, which constitutes measures to increase the ratio of the grain boundary. However, even if such measures are adopted, it is difficult to obtain an electrical resistivity exceeding 1 Ωm order as the grain itself has a low resistance, and the above-mentioned measures fall short of a thorough solution.

Further, a Mn—Zn ferrite to which, for example, CaO, SiO₂, SnO₂ and TiO₂ are added to obtain a higher resistance has been developed and is disclosed in Japanese Patent Application No. Hei 9-18092. However, the electrical resistivity of the Mn—Zn ferrite is as low as 0.3 to 2.0 Ωm, which is insufficient for application in a high frequency region. Further, a Mn—Zn ferrite containing 50 mol % or less Fe₂03 to which SnO₂ or the like is added is disclosed in EPC 1,304,237. Although it is supposedly very difficult for Fe²⁺ to be formed when Fe₂O₃ content is 50 mol % or less, the Mn—Zn ferrite described in this EPC patent contains as much as 3 to 7 mol % Fe²⁺. Therefore, the electrical resistivity of the Mn—Zn ferrite in the EPC patent cannot exceed the electrical resistivity of a conventional general Mn—Zn ferrite.

On the other hand, a Mn—Zn based ferrite which contains less than 50 mol % Fe₂O₃ for a higher resistance has been developed for use as a core material for a deflecting yoke and is disclosed in Japanese Patent Laid-Open Nos. Hei 7-230909, Hei 10-208926, Hei 11-199235 and the like.

However, judging from the fact that the application thereof is a core material for a deflecting yoke and from examples of the invention described in each publication, the Mn—Zn based ferrites described in any of the above publications are ferrite materials intended to be applied in a frequency region of 64 to 100 kHz. It is described that reason for setting the Fe₂O₃ content to 50 mol % or less for obtaining a high resistance is to make it possible to wind a copper wire directly around a core for a deflecting yoke. Thus, those publications do not suggest the application of the Mn—Zn based ferrite in such a high frequency region as exceeding 1 MHz. All the Mn—Zn based ferrites have an initial permeability of about 1100 at 100 kHz, and excellent soft magnetic properties cannot be obtained by merely setting the Fe₂O₃ content to less than 50 mol % so as to obtain a high electrical resistivity.

Further, Japanese Patent Examined Application No. Sho 52-4753 discloses a Mn—Zn ferrite containing 50 mol % or less Fe₂O₃, to which 1.3 to 1.5 mol % CoO was added in order to decrease the temperature coefficient of initial permeability. This Mn—Zn ferrite also contains as low as 11 mol % ZnO and its relative partial pressure of oxygen at sintering and cooling is not strictly controlled. Thus, the initial permeability at 100 kHz is about 2000.

SUMMARY OF THE INVENTION

The present invention has been made in consideration of the above-mentioned conventional problems, and an object of the present invention is therefore to provide a Mn—Zn ferrite which has a higher electrical resistivity than 1 Ωm order and at the same time high initial permeabilities of 4000 or more at 100 kHz and of 100 or more at 10 MHz, and a production process by which such a Mn—Zn ferrite can be obtained easily and inexpensively.

A Mn—Zn ferrite according to an aspect of the present invention to attain the above-mentioned object is characterized in that the main components include 44.0 to 49.8 mol % Fe₂O₃, 15.0 to 26.5 mol % ZnO, 0.1 to 3.0 mol % CoO, 0.02 to 1.00 mol % Mn₂O₃ and the remainder MnO.

The present Mn—Zn ferrite may contain, in addition to the above-mentioned main components, at least one of 0.010 to 0.200 mass % V₂O₅, 0.005 to 0.100 mass % Bi₂O₃, 0.005 to 0.100 mass % In₂O₃, 0.005 to 0.100 mass % PbO, 0.001 to 0.100 mass % MoO₃ and 0.001 to 0.100 mass % WO₃ as additive.

Further, the present Mn—Zn ferrite has an initial permeability of 4000 or more at 100 kHz and 100 or more at 10 MHz at room temperature (25° C.).

Still further, a production process according to the present invention to attain the above-mentioned object is characterized in that a mixed powder whose components are adjusted so as to obtain the composition of the above-mentioned Mn—Zn ferrite is pressed, then sintered and cooled, after the sintering, down to 500° C. or lower in an oxygen atmosphere with a relative partial pressure of oxygen defined by an arbitrary value selected from a range of 6 to 10 as a constant b in the expression (1).

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

In a conventional general Mn—Zn ferrite, Fe₂O₃ content is more than 50 mol % that is the stoichiometric composition, as described above. Thus, in order to prevent this excessive Fe₂O₃ from getting precipitated as hematite, sintering and cooling had to be performed under a condition where a relative partial pressure of oxygen is reduced to a significantly lower level by flowing nitrogen, that is a condition obtained with the constant b set to 7 to 8. On the other hand, since the Mn—Zn ferrite of the present invention contains less than 50 mol % Fe₂O₃, hematite is hardly precipitated. Thus, even if a range of relative partial pressure of oxygen in sintering is somewhat increased, excellent magnetic properties can be obtained. Further, in a conventional Mn—Zn ferrite that contains more than 50 mol % Fe₂O₃, about 3.0 mol % Fe²⁺ exists. On the other hand, in the Mn—Zn ferrite of the present invention, Fe 2+ content is as little as 0.1 to 0.7 mol %. Accordingly, the electrical resistivity of the Mn—Zn ferrite of the present invention is very high. Therefore, an eddy current is not increased so much even in a high frequency region, and an excellent initial permeability can be obtained. However, if this Fe₂O₃ content is too small, the saturation magnetization is deteriorated. Thus, at least 44.0mol % Fe₂O₃ is needed.

ZnO as main component influences the Curie temperature and the saturation magnetization. Too small amount of ZnO reduces the initial permeability, but on the contrary, too large amount of ZnO lowers the saturation magnetization and the Curie temperature, so ZnO content is set to the above-mentioned range of 15.0 to 26.5 mol %.

Since Co²⁺ in CoO has a positive crystal magnetic anisotropy, CoO can cancel out a negative crystal magnetic anisotropy of Fe³⁺ even if Fe²⁺ having a positive crystal magnetic anisotropy exists only in a small amount. Further, Co²⁺ has an effect of reducing the loss in a high frequency region by generating an induction magnetic anisotropy. However, when CoO content is too small, the effect is small. On the contrary, when the CoO content is too large, the magnetic strain becomes large and the initial permeability is decreased. Thus, the CoO content is set to 0.1 to 3.0 mol %.

A manganese component in the above-mentioned ferrite exists as Mn²⁺ and Mn³⁺. However, since Mn³⁺ strains a crystal lattice, thereby significantly lowering the initial permeability, Mn₂O₃ content is set to 1.00 mol % or less. However, if the Mn₂O₃ content is too small, the electrical resistivity is significantly decreased. Thus, at least 0.02 mol % Mn₂O₃ is to be contained in the ferrite.

In the present invention, at least one of V₂O₅, Bi₂O₃, In₂O₃, PbO, MoO₃ and WO₃ can be contained as additive(s). All of these additives have an action of accelerating grain growth. The initial permeability in a comparatively lower frequency region depends on its grain size, so the initial permeability in a lower frequency region can be enhanced by allowing the above-mentioned additive(s) to be contained. However, if the content thereof is too small, the effects are small. On the contrary, if the content is too large, grains grow abnormally. Accordingly, it is desirable that V₂O₅ be set to 0.01 to 0.200 mass %, Bi₂O₃, In₂O₃ and PbO be respectively set to 0.005 to 0.100 mass %, and MoO₃ and WO₃ be respectively set to 0.001 to 0.100 mass %.

In the present invention, as described above, amount of Mn3+ is controlled by conducting sintering and cooling after the sintering in an atmosphere of a relative partial pressure of oxygen obtained by using an arbitrary value in a range of 6 to 10 as a constant b in the expression (1). When a value larger than 10 is selected as the constant b, the amount of Mn³⁺ in the ferrite becomes larger than 1 mol % whereby the initial permeability is rapidly lowered. Therefore, the amount of Mn³⁺ in the ferrite must be decreased to increase the initial permeability. Thus, it is desirable that a small value be selected as the constant b. However, when a value smaller than 6 is selected, amount of Fe 2+ is increased or amount of Mn³⁺ is decreased too much whereby the electrical resistivity is significantly lowered. Accordingly, the constant b is set to at least 6.

In production of the Mn—Zn ferrite, respective raw material powders of Fe₂O₃, ZnO, CoO, Mn₂O₃ and MnO, which are the main components, are previously weighed for a prescribed ratio, and mixed to obtain a mixed powder, and then this mixed powder is calcined and finely milled. Although temperatures for the calcination may be set slightly different from each other depending on target compositions, appropriate temperatures are selected from a range of 800 to 1000° C. Further, a general-purpose ball mill can be used for the fine milling of the calcined powder. When V₂O₅ , Bi₂O₃, In₂O₃, PbO, MoO₃ and WO₃ are made to be contained as additives, proper amounts of powders of these additive are added to the fine milled powder and mixed with each other to obtain a mixture having a target composition. Then, in accordance with a usual ferrite production process, granulation and pressing are conducted, and sintering is then conducted at 1100 to 1400° C. Incidentally, in the granulation a process of adding a binder such as polyvinyl alcohol, polyacrylamide, methyl cellulose, polyethylene oxide or glycerin can be used, and in the pressing a process of applying pressure of, for example, 80 MPa or more can be used.

In the above-mentioned sintering and cooling after the sintering, a relative partial pressure of oxygen is controlled by flowing inert gas such as nitrogen gas or the like into a sintering furnace. In this case, as the constant b in the expression (1), an arbitrary value can be selected from a range of 6 to 10. Thus, the constant b has a very wide allowance as compared to the constant b (7 to 8) selected in a case where a conventional general Mn—Zn ferrite containing more than 50 mol % Fe₂O₃ is sintered, and the relative partial pressure of oxygen can be easily controlled. Further, in this case, the cooling after the sintering needs to be performed in accordance with the above-mentioned expression (1) only until the temperature gets down to 500° C. because the reaction of oxidation or reduction at a temperature lower than 500° C. can be ignored irrespective of the relative partial pressure of oxygen.

EXAMPLES Example 1

Respective raw material powders of Fe₂O₃ CoO, MnO, Mn₂O₃ and ZnO were weighed for a composition of 42.0 to 51.0 mol % Fe₂O₃, 0 to 4 mol % CoO, and the remainder including MnO, Mn₂O₃ and ZnO with a molar ratio of MnO to ZnO being 3:2 when both MnO and Mn₂O₃ are all counted as MnO, and mixed with a ball mill. Then, the mixed powder was calcined in the air at 900° C. for 2 hours and milled with the ball mill for 20 hours, and a fine milled powder was obtained. Then, this fine milled powder was adjusted with regard to the component so as to obtain the composition above mentioned and further mixed with the ball mill for 1 hour. Then, this mixture was granulated with addition of polyvinyl alcohol and pressed at a pressure of 80 MPa into toroidal cores (green compacts) each having an outer diameter of 18 mm, an inner diameter of 10 mm and a height of 4 mm. Then, the green compacts were placed in a sintering furnace where an atmosphere was adjusted by flowing nitrogen so as to have such a relative partial pressure of oxygen as obtained by setting the constant b in the expression (1) to 8, sintered at 1300° C. for 3 hours and cooled after the sintering, and samples 1-1 to 1-9 as shown in Table 1 were obtained.

Final component compositions of the respective samples 1-1 to 1-9 thus obtained were checked by a fluorescent X ray analysis, and their electrical resistivities and initial permeabilities at 100 kHz and 10 MHz were measured. The results are shown together in Table 1.

TABLE 1 Electrical Sample Main Component (mol %) Resistivity Initial Permeability No. Classification Fe₂O₃ MnO* ZnO CoO (Ωm) 100 kHz 10 MHz 1-1 Comparison 51.0 29.3 19.6 0.1 0.2 3190  1 1-2 Comparison 50.2 29.8 19.9 0.1 0.5 3660  1 1-3 Present Invention 49.8 30.1 20.0 0.1  80 4080 110 1-4 Present Invention 49.0 30.3 20.2 0.5 110 4260 140 1-5 Comparison 47.0 31.8 21.2 0 170 1980  50 1-6 Present Invention 47.0 31.2 20.8 1.0 140 4400 180 1-7 Comparison 47.0 29.4 19.6 4.0 150 2760  80 1-8 Present Invention 44.0 31.8 21.2 3.0 230 4030 170 1-9 Comparison 42.0 33.6 22.4 2.0 270 2380  90 *Mn is counted as MnO

As apparent from the results shown in Table 1, all the samples 1-3 to 1-9 each containing less than 50 mol % Fe₂O₃ have significantly higher electrical resistivities than the comparative samples 1-1 and 1-2 each containing more than 50 mol % Fe₂O₃. Further, out of these samples, the samples 1-3, 1-4, 1-6 and 1-8 of the present invention containing 44.0 to 49.8 mol % Fe₂O₃ and 0.1 to 3.0 mol % CoO obtained the initial permeabilities of 4000 or more at 100 kHz and 100 or more at 10 MHz as well.

Example 2

Respective raw material powders of Fe₂O₃, CoO, ZnO, MnO and Mn₂O₃ were weighed for a composition of 48.0 mol % Fe₂O₃, 1.0 mol % CoO, 12.0 to 27.0 mol % ZnO, and the remainder including MnO and Mn₂O₃, and mixed with a ball mill, and samples 2-1 to 2-6 shown in Table 2 were obtained by following the same production conditions as employed in Example 1. Final component compositions of the respective samples 2-1 to 2-6 thus obtained were checked by a fluorescent X ray analysis, and their initial permeabilities at 100 kHz and 10 MHz and Curie temperatures were measured. The results are shown together in Table 2.

TABLE 2 Initial Curie Sample Main Component (mol %) Permeability Temperature No. Classification Fe₂O₃ MnO* ZnO CoO 100 kHz 10 MHz (° C.) 2-1 Comparison 48.0 39.0 12.0 1.0 2960 190 190 2-2 Present Invention 48.0 36.0 15.0 1.0 4010 180 180 2-3 Present Invention 48.0 33.0 18.0 1.0 4330 170 150 2-4 Present Invention 48.0 30.0 21.0 1.0 4600 160 130 2-5 Present Invention 48.0 27.0 24.0 1.0 4430 140 100 2-6 Comparison 48.0 24.0 27.0 1.0 4220 130  70 *Mn is counted as MnO

As can be seen from the results shown in Table 2, the initial permeabilities of 4000 or more at 100 kHz and 100 or more at 10 MHz as well are obtained on the samples 2-2 to 2-6 containing 15.0 mol % or more ZnO. However, the comparative sample 2-6 containing 27.0 mol % ZnO has a low Curie temperature of 70° C., which causes a problem in practical use.

Example 3

Respective raw material powders were weighed for the same composition as in the sample 1-6 of Example 1 and mixed with a ball mill. Then, the mixed powder was calcined in the air at 900° C. for 2 hours and was further milled with the ball mill for 2 hours to thereby obtain a fine milled powder. Then, this fine milled powder was adjusted with regard to the component so as to obtain the composition specified in the above and further mixed with the ball mill for 1 hour. Then, this mixture was granulated with addition of polyvinyl alcohol and pressed at a pressure of 80 MPa into toroidal cores (green compacts) each having an outer diameter of 18 mm, an inner diameter of 10 mm and a height of 4 mm. Then, the green compacts were placed in a sintering furnace where an atmosphere was adjusted by flowing nitrogen so as to have such a relative partial pressure of oxygen as obtained by setting variously the constant b in the expression (1) to a range of 5.5 to 12, sintered at 1300° C. for 3 hours and cooled after the sintering, and samples 3-1 to 3-5 as shown in Table 3 were obtained.

The electrical resistivities and initial permeabilities at 100 kHz and 10 MHz of the samples 3-1 to 3-5 thus obtained were measured. Further, quantitative analysis of Mn₂O₃ in the respective samples was performed. The results are shown together in Table 3.

TABLE 3 Electrical Sample b Resistivity Initial Permeability Mn₂O₃ No. Classification Constant (Ωm) 100 kHz 10 MHz (mol %) 3-1 Comparison   5.5  9 4620  70 0.01 3-2 Present Invention  6  70 4700 120 0.24 3-3 Present Invention  8 140 4440 180 0.43 3-4 Present Invention 10 250 4150 180 0.81 3-5 Comparison 12 300 2810 190 1.20

As can be seen from the results shown in Table 3, all of the samples 3-2 to 3-4 of the present invention which were sintered in atmospheres of relative partial pressures of oxygen obtained by setting the constant b in the expression (1) to 6 to 10 have high initial permeabilities at 100 kHz and at 10 MHz. However, since the comparative sample 3-1 which was sintered in an atmosphere of a relative partial pressure of oxygen obtained by setting the constant b to 5.5 has the lowest electrical resistivity, it has the lowest initial permeability at 10 MHz. On the contrary, since the comparative sample 3-5 which was sintered by setting the constant b to 12 contains as much as 1.1 mol % Mn₂O₃, it has the lowest initial permeability at 100 kHz.

Example 4

Respective raw material powders were weighed for the same composition as in the sample 1-6 of Example 1 and mixed with a ball mill. Then, the mixed powder was calcined in the air at 900° C. for 2 hours and milled with the ball mill for 20 hours to thereby obtain a fine milled powder. Then, this fine milled powder was adjusted with regard to the component so as to obtain the composition specified in the above, and a given amount of V₂O₅, Bi₂O₃, In₂O₃, PbO, MnO₃ or WO₃ was added to the fine milled powder as additive, then obtained mixture was further mixed with the ball mill for 1 hour. Then, this mixture was granulated with addition of polyvinyl alcohol and pressed at a pressure of 80 MPa into toroidal cores (green compacts) each having an outer diameter of 18 mm, an inner diameter of 10 mm and a height of 4 mm. Then, the green compacts were placed in a sintering furnace where an atmosphere was adjusted by flowing nitrogen so as to have such a relative partial pressure of oxygen as obtained by setting the constant b in the expression (1) to 8, sintered at 1300° C. for 3 hours and cooled after the sintering, and samples 4-1 to 4-8 as shown in Table 4 were obtained. And average grain size and initial permeability at 100 kHz of the samples 4-1 to 4-8 thus obtained were measured. The results are shown together in Table 4.

TABLE 4 Initial Sample Additive Grain Size Permeability No. Classification (mass %) (μm) 100 kHz 1-6 Present Invention — 14 4400 4-1 Present Invention V₂O₅ 0.010 16 4490 4-2 Present Invention V₂O₅ 0.200 21 4630 4-3 Comparison V₂O₅ 0.300 Abnormal 2790 Grain 4-4 Present Invention Bi₂O₃ 0.050 20 4620 4-5 Present Invention In₂O₃ 0.050 19 4570 4-6 Present Invention PbO 0.050 17 4580 4-7 Present Invention MoO₃ 0.050 21 4700 4-8 Present Invention WO₃ 0.050 16 4510

As can be seen from the results shown in Table 4, all of the samples 4-1,4-2 and 4-4 to 4-8 of the present invention each containing a proper amount of additive have larger grain sizes and have initial permeabilities further improved, as compared with the sample 1-6 of the present invention containing no additive. However, the comparative sample 4-3 excessively containing V₂O₅ as additive incurs an abnormal grain growth, which significantly lowers the initial permeability.

As described above, the Mn—Zn ferrite of the present invention, which contains Fe₂O₃ in an amount of 44.0 to 49.8 mol %, that is less than the stoichiometric composition, also contains 0.1 to 3.0 mol % CoO and 0.02 to 1.00 mol % Mn₂O₃, and is sintered in an atmosphere of a suitable relative partial pressure of oxygen, obtains excellent initial permeabilities in a wide range of 100 kHz to 10 MHz. Thus, the utility of the Mn—Zn ferrite of the present invention is very large.

Further, when at least one of V₂O₅, Bi₂O₃, In₂O₃, PbO, MoO₃ and WO₃ is contained in proper amounts as additive, a still higher permeability can be ensured in a low frequency region and the utility is further increased.

Further, according to the production process of the Mn—Zn ferrite of the present invention, the relative partial pressure of oxygen during sintering and after sintering needs not be strictly controlled, thus largely contributing to stabilization and cost reduction in Mn—Zn ferrite production. 

What is claimed is:
 1. A Mn—Zn ferrite, characterized in that main components include 44.0 to 49.8 mol % Fe₂O₃, 15.0 to 26.5 mol % ZnO, 0.1 to 3.0 mol % CoO, 0.02 to 1.00 mol % Mn₂O₃ and a remainder MnO.
 2. The Mn—Zn ferrite according to claim 1, wherein at least one of 0.010 to 0.200 mass % V₂O₅, 0.005 to 0.100 mass % Bi₂O₃, 0.005 to 0.100 mass % In₂O₃, 0.005 to 0.100 mass % PbO, 0.001 to 0.100 mass % MoO₃ and 0.001 to 0.100 mass % WO₃ is contained as additive.
 3. The Mn—Zn ferrite according to claim 1, wherein an initial permeability at room temperature (25° C.) is 4000 or more at 100 kHz and 100 or more at 10 MHz.
 4. A production process of Mn—Zn ferrite, characterized in that a mixed powder whose components are adjusted so as to obtain the composition of the Mn—Zn ferrite according to any one of claims 1 to 3 is pressed, then sintered and cooled, after the sintering, down to 500° C. or lower in an atmosphere of a relative partial pressure of oxygen defined by the following expression: log Po ₂−14540/(T+273)+b where T is temperature (° C.), PO₂ is a relative partial pressure of oxygen, and b is a constant selected from a range of 6 to
 10. 5. The Mn—Zn ferrite according to claim 2, wherein an initial permeability at room temperature (25° C.) is 4000 or more at 100 kHz and 100 or more at 10 MHz. 